Background of the Invention
[0001] This invention relates to both a method and apparatus, as illustrated in Figure 1,
for the non-invasive determination of blood oxygen, particularly in a fetus.
[0002] Oxygen is essential to human life; for the adult, child and fetus. Asphyxia is the
condition where the lack of oxygen causes the cessation of life. Hypoxia is a deficiency
in the amount of oxygen reaching the tissues. While hypoxia is not fatal it may cause
severe neurological damage.
[0003] Methods currently available to the obstetrician and labor room staff for assessment
of fetal status include non-invasive measures such as monitoring the contraction patterns
of the expectant mother and monitoring fetal heart rate. In the presence of possible
fetal distress suggested by clinical evaluation, or non-invasive monitoring methods,
or invasive procedures such as intermittent fetal scalp blood samples (for fetal blood
pH determination), or percutaneous umbilical blood sampling (PUBS), emergent caesarean
section is often performed.
[0004] With both the non-invasive or invasive measures for determining fetal status identified
above, information concerning the most important physiological parameter of fetal
well-being, blood oxygen saturation, is not available to the physician. Changes in
fetal heart rate and blood pH are secondary manifestations of a primary condition,
fetal hypoxia.
[0005] The ability to determine blood oxygen saturation in both pediatric (including newborn)
and adult populations via oximetry, particularly pulse oximetry, is well known. Oximetry
in such applications (but not in fetal monitoring, as explained below) is an accepted
method of oxygen determination and has been utilized in clinical medicine for approximately
10 years. It is used to ensure that the patient's oxygen level is adequate to prevent
damage to organs such as the brain, heart, lungs, and kidneys.
[0006] There are two types of oximeters: (1) invasive oximeters; and (2) non-invasive pulse
oximeters. The invasive oximeters must have the light beam and detector optics in
contact with blood. In clinical medicine the sampling device, typically a fiber optic
catheter probe, is placed in a large blood vessel in the body and measurement is made
on the blood that passes by the catheter.
[0007] Non-invasive (i.e., pulse) oximeters do not require direct contact with the blood.
The non-invasive pulse oximeters are able to remove the interferences generated by
the tissue and bone, determining the difference between data from high and low pulse
pressures by performing a ratio. As only arterial blood pulses, non-invasive oximeters
only analyze arterial blood.
[0008] The prior patented technology can be broken down into three categories:
1) Non-invasive blood oxygen saturation determination instruments utilizing a transmission
sampling technique, with analysis based on two wavelengths. U.S. patent Nos. 4,770,179,
4,700,708, 4,653,498 and 4,621,643 to New et al. are believed to represent the best
examples of this technology.
2) Invasive blood oxygen saturation determination instruments utilizing a fiber optic
probe with reflectance sampling in which the probe must be inserted into a blood containing
area. U.S. patent No. 4,114,604 to Shaw et al. is believed to represent the best example
of this prior art.
3) Non-invasive blood oxygen saturation determination utilizing a reflectance method
with analysis of the reflected light by a linear algorithm employing only two wavelengths.
This technology is represented by U.S. patent No. 4,859,057 to Taylor et al.
[0009] The methods disclosed in the above-identified patents on pulse oximetry (e.g. New
et al. and Taylor et al.) are based upon several related facts. First, the concentration
of blood in a given location of the body varies with each pulse of the heart. With
each heart beat a systolic pulse pressure is generated which leads to a maximal expansion
of the vascular system. During the resting period of the cardiac cycle (i.e., diastole)
there is no pressure generated and the vascular system returns to a minimal size.
The light transmitted or reflected during diastole interacts with the skin, fat, bone,
muscle and blood. Light transmitted or reflected during systole, interacts with the
same skin, fat, bone, muscle, and blood, plus an additional amount of blood which
is present due to the expansion of the arterial system. If the diastolic signal is
subtracted from the systolic signal the result is a signal which represents the additional
amount of blood. The quality and clarity of the subtraction generated signal is related
to the amount of additional blood present which, in turn, is proportional to the pulse
pressure, (i.e., the difference between systolic pressure and diastolic pressure).
See Figure 2 for a graphical representation of the above process.
[0010] All present pulse instruments assess variations in red blood cell concentration by
utilizing a light frequency near or at the isobestic point, where measurement of pulsatile
volume is made independent of oxygen saturation. An isobestic wavelength is one which
does not change intensity with oxygen saturation but only with blood concentration.
A second wavelength in the red portion of the spectrum, which is sensitive to oxygen
saturation, is detected by either a transmission or reflection sampling technique.
By using the isobestic wavelength as a reference and by comparing its spectral intensity
to the intensity of the second wavelength in the red portion of the spectrum, it is
possible to determine the oxygen saturation of the blood non-invasively.
[0011] Oximeters based on invasive procedures also use a frequency at or near the isobestic
point. In invasive instruments the intensity at the isobestic frequency is related
to the amount of light returning or reflected by the sample which, in turn, is related
to the hematocrit (i.e., the percent volume of the blood volume occupied by red blood
cells). Basically, invasive methods simply take a ratio of the "red" wavelength divided
by the isobestic wavelength.
[0012] In all prior known applications, the algorithm used for analysis of the two, or sometimes
three, wavelengths detected have typically utilized a single analysis frequency with
a single background correction frequency to determine a single proportionality constant
describing the relationship between absorbance and concentration (i.e., univariate
or one variable algorithms). In the patents to New et al. the blood oxygen saturation
determination is made by utilizing a ratio between the ambient transmission and the
change in transmission occurring during each pulse at both wavelengths.
[0013] Shaw, et al., U.S. patent No. 3,847,483, describes non-invasive apparatus using two
wavelengths of light which originate from two alternately energized light-emitting
diodes. The oxygen saturation is then determined by an equation, which may be characterized
as a nonlinear, bivariate algorithm, employing 6 calibration constants. U.S. patent
No. 4,114,604, also to Shaw, et al., discloses what is described as an improved catheter
oximeter which operates on radiation at three or more different wavelengths.
[0014] Shaw et al. recognize the nonlinear characteristics involved in oxygen saturation
determination and recommend a possible method for overcoming this problem. It is important
to note that the Shaw methodology utilizes only a few discrete non-overlapping frequencies
taken at different non-overlapping time periods. It is also important to note that
it is not suited to non-invasive determinations as it does not disclose any method
of eliminating background components such as hair, bone and skin.
[0015] The reflectance oximeter disclosed by Taylor et al., No. 4,859,057, does not disclose
a specific mathematical relationship between the two wavelengths utilized. The method
of determining oxygen saturation requires calculation of the difference between the
minimum and maximum components of an a.c. signal. The resulting difference is then
used to determine O₂ sat. through the use of a look-up table.
[0016] An additional methodology associated with invasive reflectance determination is disclosed
by Hoeft et al., "In Vivo Measurement of Blood Oxygen Saturation by Analysis of Whole
Blood Reflectance Spectra", SPIE Vol 1067 Optical Filters in Medicine IV (1989). The
actual instrumentation utilized consists of an optical multichannel instrument that
is a grating spectrometer with a CCD array detector. They employ a simple relationship
based upon one of the two wavelength regions used being an isobestic range. Oxygen
saturation is then assumed to be a linear function of the ratio of the light intensity
reflected from the blood at the isobestic and non-isobestic wavelengths as follows:
where I₁ is light intensity diffusely scattered back from the blood at the isobestic
wavelengths (840-850 nm), I₂ is the light intensity diffusely back scattered at the
non-isobestic wavelengths (600-840 nm), and A and B are experimentally determined
calibration coefficients. The method of Hoeft et al., differs from the other above
identified methodologies in that they allow for simultaneous sampling of multiple
frequencies. Before the O₂ saturation of an unknown sample can be determined, the
hemoglobin of the blood sample must be known for the calculation of coefficients A
& B. Although Hoeft's methodology utilizes information from more than one frequency,
it uses a univariate algorithm. Additionally, Hoeft's method is not suited to non-invasive
analysis since it requires a determination of hemoglobin concentration via wet chemistry.
[0017] Over the past few years significant research has been done in the attempt to create
a clinically useful pulse oximeter for fetal monitoring, but none have been reliable
or accurate enough to reach clinical medicine. The reason for this failure is multi-factorial,
including the difficulty of the environment and the parameters under which a fetal
pulse oximeter must operate. This work has focused on modifying existing pulse oximeters
for reflectance measurement.
[0018] The work by Johnson "Monitoring the Fetus with a Pulse Oximeter",
First International Symposium on Intrapartum Surveillance, October 1990, and Gardosi "Intrapartum O₂ Saturation Trend and Acidosis", October
1990,
First International Symposium on Intrapartum Surveillance have shown that the normal fetus at time of delivery has a blood oxygen saturation
of approximately 60% or 75%, depending upon which investigators' results are accurate.
A possible reason for this discrepancy is that existing pulse (non-invasive) oximeters
are not accurate at 0₂ saturations below 75%.
[0019] The main reasons existing oximeter technology is not suitable for fetal monitoring
are: (1) the requirement that the sampling measurement be made by reflectance spectroscopy;
(2) fetal circulation has a much lower pulse pressure than that of adults; (3) the
critical range for making a decision on operative intervention will be in the 30%
to 60% oxygen saturation region; and (4) fetal heart rate is approximately twice that
of the average adult.
[0020] In comparison to transmission measurements (as used by New et al.), the use of reflectance
spectroscopy decreases the magnitude of the return signal by approximately a factor
of 10. As the signal-to-noise ratio decreases, the precision of the oxygen saturation
determination decreases.
[0021] A requirement of non-invasive arterial blood oxygen saturation determination is that
the background components be removed. To remove background components, existing non-invasive
oximeters use the difference between diastole and systole signals. The larger the
difference between systolic and diastolic, the larger the blood volume analyzed, and
the higher the signal-to-noise ratio. While the fetus is in utero, systolic pressures
are 75-80 mm Hg and diastolic pressures of 50-55 mm Hg. Thus, the difference between
diastole and systole is significantly less, approximately 20 mm Hg, in comparison
to 60 mm Hg pulse pressure in the average adult.
[0022] The environment under which the fetal pulse oximeter is required to operate is further
complicated by the low oxygen saturations it is required to determine. The accuracy
of oxygen saturation determination with known pulse oximeters becomes quite poor at
saturations of less than 75%. The source of this error is the nonlinear relationship
between oxygen saturation and reflected or transmitted light intensity. Thus, using
data reported by Chapman et al. and Severinghaus et al. with existing technology,
the oxygen saturation of the fetus cannot be determined with an error of less than
10% for the expected fetal oxygen saturations below 75%.
[0023] In summary, the physiological and physical parameters associated with fetal monitoring
represent an extreme environment under which existing oximeter technology cannot operate
with reasonable, clinically acceptable accuracy. While the articles presented at the
First International Symposium on Intrapartum Surveillance are not prior to applicants' invention, they are cited to illustrate the continued
shortcomings of existing fetal monitoring.
[0024] It is essential to realize that all prior art oximeters, both pulse and invasive,
have used 3 or less measured intensities and/or two or less variables for analysis.
Both New et al. and Shaw et al. use a limited number of wavelengths, but use nonlinear
univariate or bivariate algorithms. No algorithm is specified in Taylor. Methods that
simultaneously use two or more variables are known as multivariate methods. As used
in this application, multivariate will refer to simultaneous analysis of three or
more variables. Not only do multivariate statistical methods provide enhanced analysis
of component concentrations, but such multivariate methods have also recently made
possible the estimation of physical and chemical properties of materials from their
spectra.
[0025] A simple illustration of the increased capability of multivariate methods in component
concentration determination is provided by Figures 3A., 3B. and 3C. In Figure 3A.
one can see that an impurity component, whose spectrum overlaps that of the analyte,
can affect the spectrum of the analytic band and, therefore, the accuracy of the analysis
will suffer when the analysis is performed at a single wavelength ν₁ or when ratioing
ν₁ to a reference wavelength. The measured absorbance, A
m, at the analysis wavelength, ν₁, for a sample containing the impurity is different
than the true absorbance, A
t, of the analyte at that wavelength. If the calibration curve in Figure 3.B. is from
spectra of samples containing no impurity, then the presence of the impurity in the
sample will yield an apparent concentration that may be quite different from the true
concentration. This error will remain undetected if the intensity was measured at
only one wavelength. If the impurity is included in the calibration samples but varies
randomly in concentration in the samples, a calibration plot similar to that in Figure
3.B. will exhibit large scatter among the data, and the result will be both a poor
calibration curve and concentration estimates that have poor precision for the unknown
samples. However, with analysis at more than one wavelength, not only can the presence
of the impurity be detected, Figure 3.C., but if its presence is included in the calibration,
quantitative analysis of the analyte is possible with multivariate calibration methods,
even if the impurity and its concentration are unknown.
[0026] An indication that the unknown is different from the set of calibration samples not
containing the impurity is obtained by plotting the absorbance of the calibration
samples and the unknown sample spectra at two frequencies selected for analysis. As
exhibited in Figure 3.C., the spectrum of the sample containing the impurity (indicated
by "x") is obviously different than that of the calibration spectra (i.e. it is an
outlier). Outliers are those samples or spectra among either the calibration or unknown
data which do not exhibit the characteristic relationship between composition and
spectra of the other calibration samples. The sensitivity in detecting outliers is
increased by increasing the number of frequencies included in the analysis. The number
of independently varying impurities that can be accounted for in the analysis is also
increased by increasing the number of frequencies utilized.
[0027] Accurate univariate methods are dependent upon the ability to identify a unique,
isolated band for each analyte. Multivariate methods can be used even when there is
overlap of spectral information from various components over all measured spectral
regions. Unlike univariate methods, multivariate techniques can achieve increased
precision from redundant information in the spectra, can account for base-line variations,
can more fully model nonlinearities, and can provide outlier detection.
[0028] The general approach that is used when statistical multivariate methods are applied
to quantitative spectroscopy problems requires calibration in which a mathematical
model of the spectra is generated. See Figure 4. This calibration model can then be
used for prediction of concentrations in unknown samples. The spectra of a series
of calibration standards are first obtained, such that the spectra span the range
of variation of all factors which can influence the spectra of future unknown samples.
Assuming that the calibration uses samples that contain all the components expected
in the unknown samples and spans their expected range of variation, the calibration
will be able to empirically account for (or at least approximate) non-ideal behavior
in Beer's law, independent of the source of the non-ideal behavior. Nonlinearities
may arise from spectroscopic instrumentation, dispersion, or intermolecular interactions.
As used in this application "nonlinear" refers to any deviation in Beer's law or the
inverse Beer's law relationship (i.e., which cannot be modeled with the standard linear
expression y = mx + b; where y represents the dependent variable, x is the independent
variable, and m and b are, respectively, the slope and intercept). The spectral response
with changing oxygen saturation is not linear.
[0029] Once the empirical calibration relating spectra and component concentrations has
been performed, then the spectrum of the unknown sample can be analyzed by a multivariate
prediction step to estimate the component concentration or properties. If the calibration
samples are truly representative of the unknown sample, then the result of the analysis
will be an estimate which will have a precision similar to that found in the set of
calibration samples. In addition, spectral residuals (i.e., the difference between
measured and estimated spectra) can be used to determine if the unknown sample is
similar to the calibration samples. If the unknown sample is not representative of
the calibration samples (i.e., is an outlier) spectroscopic interpretation of the
residuals can often be made to determine the source of any differences between unknown
and calibration samples.
[0030] The multivariate methods which are best suited for analysis of oximeter data are
those that model the spectra using an inverse Beer's law model, such as principal
component regression (PCR) or partial least squares (PLS). In an inverse Beer's law
model the concentration of each component in the mixture is represented as a linear
function of the sampled absorbance spectrum. An advantage of this multivariate approach
is that the nonlinearities in the spectral response to changes in composition can
be accommodated without the need for an explicit model. For the chemical components
to be predicted, PCR or PLS analysis is used to construct a linearly independent set
of factors based upon a set of calibration spectra (i.e., spectra for which the composition
to be predicted is known). The number of these component factors which are useful
for prediction (the "rank" of the model) is selected by a cross-validation procedure,
which is also used to estimate the precision of subsequent predictions. PLS and PCR
methods are capable of achieving accurate and precise results in the presence of linear
and nonlinear dependencies in the absorbance spectrum at various frequencies. Thus,
an entire spectral region can be used in multivariate analysis without the need for
the spectroscopist to choose an optimal set of wavelengths for the analysis. Similarly,
these methods of computation are not sensitive to linear dependencies introduced by
over sampling of information at many frequencies in the construction of the calibration
samples.
[0031] U.S. patent No. 4,975,581 to Robinson et al. discloses a method and apparatus for,
particularly, quantitatively determining the amount of glucose in a human. The method
relates to determining one or more unknown concentration values of a known characteristic
(e.g. glucose) via the steps of:
a. Irradiating a biological fluid (i.e., blood) having unknown values of a known characteristic
(i.e., glucose) with infrared energy having a least several wavelengths so that there
is differential absorption of at least some of the wavelengths by the biological fluid
as a function of both the wavelengths and the known characteristic.
b. Measuring the absorption variations from the biological fluid.
c. Calculating the unknown values of the known characteristic (i.e., glucose) in the
biological fluid from the measured absorption variations utilizing a multivariate
algorithm and a mathematical calibration model. The model is constructed from the
set of samples and is a function of the known values of the characteristic and the
intensity variations vs. wavelengths information obtained from irradiating the set
of samples.
[0032] The method can be used in vivo and non-invasively, in vivo and invasively, and in
vitro.
[0033] The applicants recognize that the preferred embodiment of U.S. patent No. 4,975,581
utilizes the partial least squares algorithm. However, the reasons for utilizing the
PLS algorithm in the present invention are quite different from the reasons it was
utilized to determine glucose concentrations. The limiting factor in the determination
of a blood analyte, such as glucose, is the lack of information available. The determination
of a blood analyte requires a very high signal-to-noise ratio and a sophisticated
algorithm for extraction of a minuscule amount of information (glucose is, normally,
0.1 weight percent of blood). In the case of a pulse oximeter suitable for fetal monitoring,
the information is abundant, but the environment of operation is extreme. As has been
previously mentioned, the reflected light-oxygen saturation relationship is highly
nonlinear, the signal for analysis is extremely noisy and the present invention must
remove the interfering background components by correlating with the pulsating blood.
Also the frequency regions used for analysis are separate and the basic instrumentation
is different.
[0034] Despite past and continuing failures, an accurate assessment of fetal oxygen saturation
can be obtained by measuring the peripheral blood oxygen saturation in the fetus.
The technology for the realization of this goal, no more invasive than the electronic
heart monitors currently used, is disclosed herein. This improved method and apparatus
should lead to a reduction in the rate of Cesarean sections for apparent fetal distress.
Such a monitor should improve the survival rate of otherwise compromised fetuses by
early and accurate detection of real problems. Thus, the ultimate goal of a healthy
mother and baby will be enhanced.
[0035] It is an object of the present invention to provide a fetal oximeter which can easily
and accurately operate in the extreme environment of fetal monitoring, thus overcoming
the shortcomings of existing technology.
[0036] The object of the pulse oximeter of the present invention is to overcome the limitations
of prior art oximeters, including their inability to obtain information at a variety
of wavelengths simultaneously, and the limitation inherent in the time necessary for
the intermittently energized light sources in such prior art oximeters to reach the
required brightness and stability.
[0037] In contrast to Shaw et al., another object of the present invention is to utilize
multiple frequencies with simultaneous sampling, employ an algorithm which can model
nonlinearities over the entire clinically observed blood oxygen saturation range and
which is suitable for non-invasive measurements in the fetus' environment.
[0038] It is another and important object to determine if a sample's spectrum and subsequently
determined oxygen value is representative of the calibration samples. This is crucial
for the implementation of an accurate and reliable clinical instrument. Identifying
and removing outlier samples from the calibration set will drastically improve the
accuracy and precision of the analysis. Identification of outliers among the unknown
samples provides information for evaluating the validity of the fetal blood oxygen
saturation determination. This ability is especially important in this medical application
because the consequences of hypoxia on the fetus can result in death or lifelong disability.
According to the present invention, utilization of a pulse oximeter employing outlier
detection methods would result in the generation of a "flag" when analyzing a spurious
sample, indicating that the analysis was unreliable.
[0039] It is another object of the invention to provide an oximeter based on a multivariate
inverse Beer's law model, such as PLS or PCR, to provide the following benefits:
a. Accommodation for nonlinear spectral responses without a degradation in prediction
accuracy;
b. Compensation for the presence of interferences of undetermined origin (e.g., chemical
contaminants or physiological variations); and
c. Identification of spurious or outlier samples in both the calibration samples and
in the unknown samples.
[0040] No simple or obvious combination of the prior art will result in an instrument capable
of non-invasively and accurately monitoring fetal oxygen saturation over wide ranges
of saturation values. For instance, existing oximeters do not measure multiple wavelengths
simultaneously. Therefore, the full advantages of using a powerful multivariate algorithm
like PLS could not be obtained due to the limited number of frequencies available
when using existing instrumentation. Though Taylor, et al., discloses reflectance
sampling, all known commercially available pulse oximeters use transmission sampling.
Further, conventional oximeters do not use gratings or any mechanism that separates
light into its constituent wavelengths.
[0041] The present invention represents a significant advancement in apparatus and methodology
by:
a. Simultaneous and rapid sampling at multiple frequencies. Rapid sampling is necessary
due to the rapid rate of the fetal heart and large variations in beat-to-beat pulse
pressure. To distinguish the true maximum and minimum of the vascular system, a sampling
rate ≧ 50 Hz would be desirable, and is feasible using our technology.
b. Use of an emitter/detector apparatus, in connection with fiber optics, which is
well-suited for attachment to the fetus for reflection sampling.
c. Analysis of the spectral information with a multivariate algorithm. A multivariate
analysis will be superior to either univariate or bivariate analyses because the information
available at multiple frequencies can be combined to yield more information with a
higher precision and reliability than the information available at one or several
discrete frequencies or ratios. The preferred algorithms are known as partial least
squares (PLS) and principle component regression (PCR). Other suitable algorithms
are classic least squares (CLS), Q-matrix method, cross correlation, Kalman filtering
and multiple linear regression (MLR). MLR is sometimes referred to as inverse least
squares (ILS).
d. Providing the doctor with a measure of validity or an assurance of accuracy by
employing outlier detection methods. The ability to identify false negatives is extremely
important because the consequences of hypoxia on the fetus can result in death or
life-long neurological deficits. On the other hand, the ability to eliminate false
positives will reduce the incidence of unnecessary caesarean sections, a surgical
intervention with risks for both fetus and mother.
Summary
[0042] A method and apparatus for determining non-invasively and in vivo the blood oxygen
level in a mammal, particularly a fetus. The method includes the step of simultaneously
generating a plurality of different wavelengths of light in the range of 500 nm to
1,000 nm. The wavelengths of light are used to irradiate in vivo and non-invasively
blood containing tissue having an unknown blood oxygen level during the diastolic
portion of the cardiac cycle so that there is differential attenuation of at least
some of the wavelengths by the blood containing tissue as a function of the wavelengths.
The differential attenuation causes intensity variations of the wavelengths incident
from the blood containing tissue as a function of the wavelengths, the tissue and
the unknown blood oxygen level. The intensity variations from the blood containing
tissue during the diastolic portion are simultaneously measured to obtain a diastolic
set of intensity variations v. wavelengths. The wavelengths of light are also used
to irradiate in vivo and non-invasively the blood containing tissue during the systolic
portion of the cardiac cycle, so that there is attenuation of at least some of the
wavelengths by the blood containing tissue as a function of the wavelengths. The differential
attenuation causes intensity variations of the wavelengths incident from the blood
containing tissue as a function of the wavelengths, the tissue and the unknown blood
oxygen level. The intensity variations from the blood containing tissue during the
systolic portion are also simultaneously measured to obtain a systolic set of intensity
variations v. wavelengths. Finally, the method includes the step of calculating the
value of the unknown blood oxygen level in the blood containing tissue from the measured
intensity variations during the diastolic portion and the systolic portion of the
cardiac cycle utilizing an algorithm and a calibration model. The algorithm is a multivariate
algorithm using 3 or more variables and is capable of modeling at least some nonlinearities
over the entire clinically observed range of blood oxygen levels. The model is constructed
from a set of calibration samples in which the blood oxygen levels are known, and
are a function of the known oxygen levels and the intensity variations v. wavelengths
obtained from irradiating the set of calibration samples with a plurality of different
wavelengths of light in the range of 500 nm to 1,000 nm.
[0043] Preferably, the method also includes the step of determining whether the intensity
variations v. wavelengths from the blood containing tissue having an unknown blood
oxygen level represent an outlier. The method also includes the step of determining
whether any of the calibration samples from the set of samples is a spectral or a
concentration outlier. Optionally, the method may further include the steps of pretreatment
of the measured intensity variations, and pretreatment of the blood oxygen level.
The algorithm is selected from the group including PLS, PCR, CLS, Q-matrix method,
cross correlation, Kalman filtering and MLR. Preferably the algorithm used has decreased
sensitivity to noise by signal averaging the effects of intensity variations v. wavelengths
when there are more intensities than independent sources of spectral variation, particularly
PLS and PCR. The method may also include the step of modifying the intensity variations
v. wavelengths response from the blood containing tissue to account for the amount
of hemoglobin present in the blood containing tissue. Finally, the method may include
the step of determining the difference between the diastolic set of intensity variations
v. wavelengths and the systolic set of intensity variations v. wavelengths from the
blood containing tissue. The determination of the diastolic portion and the systolic
portion of the cardiac cycle is done by concurrently measuring the electrical activity
of the heart.
[0044] The oximeter includes apparatus for simultaneously generating a plurality of different
wavelengths of light in the range of 500 nm to 1,000 nm; apparatus for simultaneously
directing at least a portion all of the wavelengths of light to a section of blood
continuing tissue of a mammal having an unknown oxygen level; apparatus for simultaneously
collecting at least a portion of the wavelengths of light which are directed from
the blood containing tissue; apparatus for simultaneously measuring the intensity
of each of the wavelengths collected; apparatus for storing the measured intensity
variations v. wavelengths; a calibration model generated by a multivariate algorithm
using 3 or more variables and which is capable of modeling at least some nonlinearities;
apparatus for storing the multivariate algorithm which utilizes the calibration model
and the stored intensity variations v. wavelengths for determination of the unknown
blood oxygen saturation level; a microprocessor; and apparatus for indicating the
calculated blood oxygen level.
Brief Description of Drawings
[0045]
Figure 1 is a schematic illustration of the preferred embodiment of the invention;
Figure 2 is a graphical representation of the basic principle of how a conventional
pulse oximeter obtains the "additional" blood signal;
Figure 3 is a series of graphs comparing univariate calibration to multivariate calibration;
Figure 4 is a chart showing the general approach used in multivariate statistical
methods to generate a mathematical calibration model and to use this model to quantitatively
determine concentrations and/or properties from the spectra of unknown samples;
Figure 5 is a schematic of the test apparatus of the present invention;
Figure 5A is an enlarged view of the fiber optic bundle of Figure 5;
Figure 6 is a graph illustrating the raw data (reflectance intensity vs. wavelength)
obtained at various O₂ saturations with the apparatus of Figure 5;
Figure 7 is a graph illustrating the analysis of the raw data with the algorithm of
New, et al.;
Figure 8 is a graph illustrating the nonlinear relationship between a ratio of reflected
light ratios, as specified by New, et al, and oxygen saturation;
Figure 9 is a graph illustrating the analysis of the raw data with the algorithm of
Hoeft, et al.;
Figure 10 is a graph illustrating the analysis of the raw data with the algorithm
of Shaw, et al.;
Figure 11 is a graph illustrating the correlation between O₂ saturation and frequency
and comparing the frequencies utilized by New, et al., Shaw, et al., and the multivariate
algorithms of the present invention.
Figure 12 is a plot of measured oxygen saturation vs. oxygen saturation predicted
by the principle component regression (PCR) algorithm;
Figure 13 is a plot of measured oxygen saturation vs. oxygen saturation predicted
by the partial least squares (PLS) algorithm;
Figure 14 is a graph illustrating the addition of random noise to a single-beam spectrum
corresponding to a sample with O₂ saturation of 70% and a hematocrit (HCT) of 35%;
Figure 15 is a plot of measured oxygen saturation vs. oxygen saturation predicted
by the analysis of single-beam spectra (with noise added) with the algorithm of New,
et al.;
Figure 16 is a plot of measured oxygen saturation vs. oxygen saturation predicted
by the analysis of single-beam spectra (with noise added) with the algorithm of Hoeft,
et al.;
Figure 17 is a plot of measured oxygen saturation vs. oxygen saturation predicted
by the analysis of single-beam spectra (with noise added) with the algorithm of Shaw,
et al.;
Figure 18 is a plot of measured oxygen saturation vs. oxygen saturation predicted
by the analysis of single-beam spectra (with noise added) with the PCR algorithm;
Figure 19 is a plot of measured oxygen saturation vs. oxygen saturation predicted
by the analysis of single-beam spectra (with noise added) with the PLS algorithm;
and
Figure 20 is a graphical representation of the electrical activity of the heart and
its temporal relationship to the pressure or size of the vascular system.
Description of the Preferred Embodiment
[0046] To demonstrate the nonlinear reflected light response of the blood at various oxygen
levels, the effect of physiological hematocrit variation, the inadequacies of the
algorithms used in current oximeters, and the superiority of multivariate analysis,
a set of human blood samples were examined using reflectance spectroscopy. The samples
were examined at hematocrit levels ranging from 25% to 47% and with oxygen saturations
ranging from 30% to 100%. Standard blood bank solutions of packed red blood cells
were used to create solutions with different hematocrits. The solutions of packed
red blood cells were diluted with normal physiological saline to create hematocrit
levels commonly encountered in clinical medicine. The four hematocrit levels examined
were 47%, 35%, 33% and 25%.
[0047] Each of the blood solutions at the above identified hematocrit levels was placed
in a tonometer which allowed controlled oxygenation of blood while maintaining normal
physiological temperature (i.e. 37°C/98.6° F). The blood solutions were gently stirred
to prevent settling or separation of the blood components and to provide adequate
mixing. The rotational speed of the tonometer stir rod was minimized to prevent cell
lysis.
[0048] The oxygenation of the blood was performed using a gaseous mixture of nitrogen, oxygen
and carbon dioxide. The percentages of oxygen and nitrogen were varied to provide
adequate changes in the oxygen saturation of the blood solution. The percentage of
carbon dioxide was maintained throughout the experiment at a physiological level of
between 4 and 8%.
[0049] Data were obtained by first establishing an appropriate hematocrit level and then
varying the oxygen saturation from approximately 30% to 100%, as explained above.
For each oxygen saturation examined, a 4 ml blood sample was removed from the tonometer
utilizing a standard sealed syringe. A 2 ml amount of sample was placed immediately
in a glass cuvette, and the syringe with the remaining 2 ml was capped. The syringe
was then placed on ice to prevent changes in oxygen saturation during transport to
a laboratory for conventional blood gas analysis. The oxygen saturation determination
was performed on a Radiometer OSM3 Hemoximeter.
[0050] For each oxygen saturation examined, the 2 ml which had been placed in the glass
cuvette was examined in reflectance with the test apparatus 11 illustrated in Figure
5. Apparatus 11 includes a spectrometer 13, a cuvette holder 15 and a computer 17.
Spectrometer 13 includes a halogen light source 21, a concave focusing mirror 23,
a fiber optic housing 25, a second fiber optic housing 27, a grating 29, an array
detector 31, and instrument electronics 35. Spectrometer 13 is connected to cuvette
holder 15, via fiber optic bundle 37, and to computer 17, via cable 39. Cuvette holder
15 includes a base 41, having a first or cuvette supporting arm 43 and a second arm
45. Arm 43 includes a cavity 47 for receiving and properly positioning a standard
laboratory cuvette 49. Arm 45 includes an opening 51, through which passes fiber optic
bundle 37, and supports a pair of compression springs 53 and 55. The right-hand end
57 of bundle 37, which is accurately squared off, is securely contained in a rigid
sleeve 59 which, in turn, is held in bracket 61 via set screw 63. Springs 53, 55 hold
end 57 with reproducible contact against spacer slide 65 which, in turn, is passed
into contact with one of the sides of cuvette 49. Computer 17 includes a microprocessor
and associated electronics 71, video monitor 73, disk drive 75, and a key board 77.
As illustrated in Figures 5 and 5A, bundle 37 includes a central illumination or input
fiber 81 and a surrounding bundle of receiving or output fibers 83.
[0051] Again, with reference to Figure 5, quartz-halogen light source 21, generating light
in the 500 nm to 1000 nm frequency region, is coupled into fiber optic bundle 37 to
provide illumination of sample 85. The central fiber 81 serves as the illumination
fiber while surrounding fibers 83 serve as receivers for transporting the reflected
light from the sample back to spectrometer 13. The reflected light is then separated
by frequency using a standard grating spectrometer and recorded utilizing a charge
coupled device (CCD) array detector 31, specifically a Phillips module type 56470
CCD detector array, at frequencies from 500 to 1000 nm. The detector was scanned 128
times for a total scan time of approximately one minute, with the intensity values
from a given frequency subsequently coadded to improve the signal-to-noise ratio.
The resulting intensity values at each frequency (i.e. single-beam spectral values)
were then stored on a computer disk without further manipulation, to serve as the
data set for subsequent analysis.
[0052] The process of establishing a hematocrit and then varying the oxygen saturation for
such hematocrit was performed a number of times at each of the hematocrit levels previously
identified (i.e. 47, 35, 33, 25%). Approximately 25 samples were obtained at each
hematocrit level with the oxygen saturation values of these samples being distributed
from 30% to approximately 100% saturation. The raw data is illustrated in Figure 6.
[0053] The data set obtained with the apparatus of Figure 5 was then analyzed using a variety
of algorithms which represent: (1) algorithms presently utilized on commercially available
oximeters and described in prior art patents; (2) algorithms published in the current
literature; and (3) multivariate algorithms not previously utilized for oxygen saturation
determination. The specific algorithms and how they will be referenced are:
(1) Single ratio method as described by New et al. in U.S. patent No. 4,653,498;
(2) Sum of intensities ratio method, as described by Hoeft et al.;
(3) Multiple ratio method as described by Shaw et al. in U.S. patent No. 4,114,604;
(4) Principle component regression (PCR), not previously utilized in oxygen saturation
determination; and
(5) Partial least squares (PLS), not previously utilized in oxygen saturation determination.
Single Ratio Method
[0054] The single ratio method describes the development of a linear regression using four
constants based on a ratio of intensities at 660 nm and 940 nm. Because New et al.
specify the light sources as light emitting diodes (LEDs), which emit a narrow range
of frequencies about their center frequency, the intensity value used for a given
frequency was the average intensity value of several surrounding frequencies. To model
the method and apparatus of New et al., the 660 nm intensity value was calculated
as the average of the single-beam intensities from 658 nm to 662 nm, (i.e. 5 intensity
values). The value for 940 nm was obtained from 938 nm to 942 nm in a similar manner,
again using 5 intensity values.
[0055] In New et al. the equation for determination of the regression constants is:

New et al., specify using four different saturation values and their corresponding
intensity values for determination of the regression constants (i.e., K
B2, K
B2, K
A1, K
A2). This represents a condition of four equations and four unknowns. For actual determination
of the coefficient values, one of the four coefficients must be arbitrarily set, typically,
to 1.0. This method of coefficient determination is feasible, but a better method
to determine the constants is to utilize the intensity ratios from all calibration
samples and their corresponding saturation values, and create a situation where there
are many more equations than unknowns. In a condition with more equations than unknowns,
a nonlinear least squares regression analysis can be performed to minimize error.
We determined the constants using the modified Gauss-Newton method for the fitting
of nonlinear regression functions by least squares. The analysis was performed separately
at each individual hematocrit (and at all oxygen saturation levels for each hematocrit),
and then upon the entire data set including all hematocrits and oxygen saturation
levels together. The results are shown in Figure 7 where Predicted Oxygen Saturation
was determined by the modified Gauss-Newton method, and Measured Oxygen Saturation
was determined with the Radiometer OSM3 Hemoximeter. The average errors are set forth
in Table 1.
Table 1
Hematocrit |
Average Absolute Error of Percent Oxygen Saturation |
25% |
4.4 |
33% |
11.1 |
35% |
8.4 |
47% |
4.2 |
all together |
8.9 |
Intensity sum Ratio Method
[0056] The method as described by Hoeft et al. consists of a simple linear regression based
upon a ratio of the sum of the intensities from 600 nm to 840 nm, R
sig, and a second sum of the intensities from 840 to 850 nm, R
ref. Specifically, R
sig is the sum of 289 intensity values corresponding to frequencies between 600 nm and
840 nm, and R
ref is the sum of 13 intensity values from 840 nm to 850 nm. The relation is stated as:
where A and B are hematocrit dependent. Utilizing the data set obtained from the apparatus
of Figure 5, a linear regression was performed on each hematocrit group individually
and on the four different hematocrit groups combined together. The results are as
illustrated in Figure 9. The average errors are set forth in Table 2.
Table 2
Hematocrit |
Average Absolute Error of Percent Oxygen Saturation |
25% |
2.9 |
33% |
3.1 |
35% |
3.1 |
47% |
2.6 |
all together |
5.3 |
Multipie Ratio Method
[0057] The U.S. patent No. 4,114,604 to Shaw et al. describes the use of multiple ratios
utilized in a nonlinear function. The specific ratios described are R₁= (intensity
at 669 nm)/(intensity at 698 nm) and R₂ = (intensity at 798 nm)/(intensity at 698
nm). Again the specific intensity values used in our analysis were the average of
5 data values surrounding the specific frequency desired. Shaw et al. propose a rational
function model of the form

Where S is the percent oxygen saturation, the Ai's and Bi's (8 total) are model parameters,
all of which have to be estimated. Shaw et al. recommend certain constraints among
the parameter estimates, such as

and

. Shaw et al. also suggest that the parameter estimates should be selected such that
the partial derivative of the above equation with respect to R₁ should be zero near
one extreme of S, while the partial derivative of S with respect to R₂ should be zero
near the other extreme of S. If all four of these constraints are used, then there
are essentially four parameters remaining in the model. However, Shaw et al. do not
provide other details on how to estimate the model parameters. In trying to construct
a model according to Shaw's recommendations, the constraints on A₃ and B₃ were easily
incorporated into the original model. It was also necessary to set the value B₀ at
1 to obtain a model in which

where S
i is the model prediction associated with the i
th observation, and R
1i and R
2i are the observed values of the spectral ratios (R₁ and R₂) associated with the i
th observation.
[0058] The parameter estimates (with associated standard errors in parentheses) associated
with the data set (involving data from all hematocrits) over the saturation from 30%
to, approximately, 100% are
A₀ = 46.6 (38);
A₁ = -105 (89);
A₂ = 64.5 (53);
B₁ = -2.13 (.10); and
B₂ = 1.19 (.11).
[0059] Estimation of the model parameters was made by nonlinear least-squares regression
using the Gauss-Newton method. These parameter estimates are very highly correlated.
This probably indicates that the model contains more fitted parameters than necessary,
with a potential hazard that errors in the calibration data will be excessively incorporated
into the model. The analysis for each hematocrit individually and for all the hematocrits
grouped together is illustrated in Figure 10. The average errors are set forth in
Table 3.
Table 3
Hematocrit |
Average Absolute Error of Percent Oxygen Saturation |
25% |
1.4 |
33% |
1.2 |
35% |
1.2 |
47% |
0.9 |
all together |
2.7 |
Multivariate Analysis
[0060] There are four full-spectrum multivariate algorithms (PLS, PCR, CBS and MLR/ILS)
commonly used in spectroscopy. We have determined that the two methods best suited
for accurate determination of oxygen saturation in a fetus are PLS and PCR.
[0061] To explain the superiority of full-spectrum multivariate algorithms one needs to
understand that: (1) information on oxygen saturation is present at multiple frequencies,
(2) full-spectrum multivariate methods have a signal averaging effect, and (3) some
multivariate methods (particularly PLS and PCR) can accommodate nonlinear spectral
responses. Examination of Figure 11, the graph of Correlation (between O₂ saturation
and frequency) vs. Frequency, reveals that the correlation is in excess of 0.80 from
600 nm to 710 nm. In contrast, for frequencies above 850 nm, the correlation is less
than 0.10. For purposes of comparison, Figure 11 also shows the frequency regions
used by New et al., Shaw et al. and the multivariate algorithms. Please note that:
(1) the frequency regions used by Hoeft are not shown on the figure; and (2) the height
of the various shaded regions is arbitrary. Also note that the widths illustrated
for New et al. and Shaw et al. are wider than actually disclosed in these two references.
[0062] As illustrated in Figure 11, our inclusion of all intensities in the spectral region
(in contrast to the discreet limited regions utilized by the prior art) is beneficial
to the analysis because most of these intensities contain considerable amounts of
information relating to oxygen saturation. The multivariate full-spectrum signal averaging
effect arises from the fact that information about each analyte or property is contained
at many wavelengths and the statistical analysis serves to simultaneously use all
this information. In addition a spurious data point at a given wavelength will be
only one of many data points included in the analysis and its influence in the analysis
will be diminished. Thus, the relative weight of the intensity of a particular frequency
is decreased, and its adverse effect on the quantitative analysis is minimized.
[0063] An additional advantage of multivariate methods is their ability to model nonlinear
relationships between the spectra and concentration. Our experience in determining
blood oxygen saturation using reflected light has demonstrated that the relationship
between reflected light intensity and oxygen saturation is nonlinear. The sources
of this nonlinearity are at least partially due to instrument/detector nonlinearities
and the sigmoidal oxygen-hemoglobin binding curve.
[0064] In summary, the physiological and physical difficulties associated with fetal monitoring
such as low pulse pressure and the necessity for reflectance sampling, which result
in decreased signal-to-noise ratios and the nonlinear relationship between saturation
and reflected light intensity, have led us to the conclusion that the utilization
of full spectrum multivariate analysis, as set forth herein, is the correct approach.
Analysis of the experimental data with multivariate methods and comparison with prior
art algorithms demonstrates the superiority of our methodology and the associated
instrumentation.
[0065] Principal component regression (PCR) and partial least squares (PLS) are similar
methods of multivariate analysis. Both are factor analysis methods which are full
spectrum in nature; both can model some nonlinearities; and both allow for detection
of outliers. PLS and PCR can be employed even when the concentrations or properties
of only one component are known in the calibration samples.
Principle Component Regression
[0066] Analysis of the single-beam spectral data by PCR was performed for each hematocrit
individually and then upon the entire data set (i.e., all hematocrits together). The
results of the analysis are as illustrated in Figure 14. The average errors are set
forth in Table 4.
Table 4
Hematocrit |
Average Absolute Error of Percent Oxygen Saturation |
25% |
1.8 |
33% |
1.2 |
35% |
1.2 |
47% |
0.4 |
all together |
2.3 |
Partial Least Squares
[0067] The analysis of the single beam spectral data by PLS was, like PCR, preformed for
each hematocrit individually and then upon the entire data set (i.e., all hematocrits
together). The results of the analysis are illustrated in Figure 15. The average errors
are set forth in Table 5.
Table 5
Hematocrit |
Average Absolute Error of Percent Oxygen Saturation |
25% |
0.6 |
33% |
1.2 |
35% |
1.0 |
47% |
1.6 |
all together |
2.0 |
Analysis with the Addition of Noise
[0068] As has been discussed previously, the fetal environment represents a condition in
which the "additional" blood spectrum will have poor signal-to-noise ratio characteristics.
The experimental spectral data used for the comparison analysis set forth above, was
acquired in a manner to minimize noise. Specifically, the blood sample was scanned
128 times and the reflectance intensity values at a given wavelength were subsequently
averaged to minimize random noise.
[0069] To simulate the noise level anticipated when monitoring an actual fetus, random computer
generated noise was added to the original data. Thus, the anticipated fetal spectral
noise was added at a level of 30% of the average maximum value of all the spectra,
and the intensity values at all wavelengths were subjected to the same magnitude and
distribution of random noise. Figure 16 sets forth a visual presentation on the amount
of noise added. The specific spectrum shown corresponds to an O₂ saturation of 70%
and a hematocrit of 35%. The resulting noisy spectral data, from all data points,
were then analyzed using the same algorithms as described above. The analysis of the
noisy data were done in exactly the same way as the original data. The results of
the analysis, which are shown below, clearly demonstrate the superiority of multivariate
analysis.
[0070] The New et al. algorithm was applied to the noisy spectra in the manner as previously
described. As can be seen from Figure 17, the results of the analysis did not have
any predictive value. The actual results are summarized below:
Table 6
Hematocrit |
Average Absolute Error of Percent Oxygen Saturation |
25% |
16.5 |
33% |
13.2 |
35% |
11.3 |
47% |
19.7 |
all together |
16.0 |
[0071] The Hoeft et al. algorithm was applied to the noisy spectra in the same manner as
previously described. Again, the results of the analysis did not have any predictive
value. See Figure 18. The actual results are summarized below:
Table 7
Hematocrit |
Average Absolute Error of Percent Oxygen Saturation |
25% |
16.0 |
33% |
11.0 |
35% |
9.2 |
47% |
18.1 |
all together |
13.6 |
[0072] The Shaw et al. algorithm was also applied to the noisy spectra in the manner as
previously described with regard to non-noisy data. As with New et al. and Hoeft et
al., and as illustrated in Figure 19, the results of the analysis did not have any
predictive value. The actual results are summarized in Table 8.
Table 8
Hematocrit |
Average Absolute Error of Percent Oxygen Saturation |
25% |
15.5 |
33% |
12.7 |
35% |
8.0 |
47% |
14.5 |
all together |
13.6 |
[0073] The principle component regression algorithm was applied to the noisy spectra in
the manner as previously described. In contrast to New et al., Hoeft et al. and Shaw
et al., the results of the analysis, illustrated in Figure 20, showed only a mild
decrease in predictive ability. Thus the PCR algorithm still performed well. The actual
results are summarized below:
Table 9
Hematocrit |
Average Absolute Error of Percent Oxygen Saturation |
25% |
3.7 |
33% |
3.4 |
35% |
3.8 |
47% |
4.2 |
all together |
5.8 |
[0074] Finally, the partial least squares algorithm was applied to the noisy spectra in
the manner as previously described. The results of the analysis showed a mild decrease
in predictive value but the algorithm still preformed well, especially given the level
of noise added to the spectral data. See Figure 21. The average absolute error of
prediction changed from 2.0 percent O₂ saturation using the non-noisy spectra to 2.6
percent O₂ saturation on the noisy spectra. The actual results are summarized below:
Table 10
Hematocrit |
Average Absolute Error of Percent Oxygen Saturation |
25% |
3.1 |
33% |
2.9 |
35% |
3.4 |
47% |
3.5 |
all together |
2.6 |
The Preferred Embodiment
[0075] With reference to Figure 1, oximeter 111 includes a spectrometer 113, an electronics
and computer processing module 115, and a visual display module 117. Spectrometer
113 includes a broad band halogen light source 121, a concave focusing mirror 123
a fiber optic housing 125, a second fiber optic housing 127, a grating 129, a CCD
array detector 131, and an electric buss 135. Module 115 includes a microprocessor
141, memory 143 in which the multivariate calibration model is stored, and module
145 in which the outlier defection algorithm is stored. Microprocessor 141, memory
143 and module 145 are connected together via suitable electronic connectors, as illustrated
schematically at 147. Visual display module 117 includes a blood oxygen saturation
display 151, heart rate display 153, an indicator of accuracy of determination 155,
oxygen saturation trend 157, and heart rate tracing 159. Finally, apparatus 111 includes
a fiber optic bundle 161, including a central control input fiber 163, and a surrounding
bundle of output fibers 165. In cross section bundle 161 has the configuration illustrated
in Figure 5A. The end of bundle 161 is secured to the scalp of the fetus via a suitable
suction or other device.
[0076] Source 121 emits frequencies from approximately 500 mm to 1000 mm, as illustrated
in Figure 11. This light is transmitted to the fetus via input fiber 163 to illuminate
a blood containing part of the fetus, such as the scalp illustrated in Figure 1. The
back scattered or reflected light is then transmitted back to spectrometer 113 by
fiber bundle 165. Alternately the same optical fiber or a secondary optical fiber
could be utilized. The returning light is then separated into various frequencies
and detected by the charge coupled device (CCD) array detector 131.
[0077] The reflected light intensities at the various frequencies are then analyzed by computer
141 employing a multivariate algorithm (such as PLS or PCR) utilizing information
over the entire spectral range. The spectral data are analyzed to establish which
spectra correspond with maximum concentration of blood (or maximum dilation) in the
arterial system of the fetus, and which spectra correspond with minimum concentration
or dilation of the arterial system. The spectra associated with minimum dilation will
contain information on blood, skin, bone, etc. The spectra associated with maximum
dilation will contain the same information plus an additional amount of blood information.
However, because reflected light does not necessarily follow a Beer's law model, data
treatments or spectral transformations for reflection spectra may be different than
for absorption spectra. Normally, diffusely reflected light is expected to follow
the Kubelka-Munk equation as follows:
where R
∞ is the absolute reflectance of an "infinitely thick" layer, s is the scattering coefficient,
and k is the molar absorption coefficient. However, the log of the inverse reflectance
sometimes yields superior quantitative results. Subtraction of the appropriately transformed
spectral data from the maximum and minimum dilation will correspond to the additional
amount of blood present due to the pulse pressure generated by the heart. The above
process effectively subtracts out the interfering background and provides the multivariate
algorithm with a spectrum corresponding to the additional blood. The subtracted spectrum
is analyzed by a multivariate algorithm. In the preferred embodiment the algorithm
employed would be partial least squares or principle component regression. The algorithm
will provide the operator with blood oxygen saturation as indicated by 151.
[0078] An additional embodiment of the invention includes apparatus for obtaining information
regarding the electrical activity of the fetal heart, which activity can provide information
to assist in determination of maximal and minimal dilation. With reference to Figure
23, maximum expansion of the arterial system due to ventricular contraction occurs
at a set interval following the R peak of the QRS complex. This complex precedes ventricular
contraction which results in ejection of blood from the heart. Minimum expansion of
the arterial system is present prior to ventricular contraction and corresponds to
a time period in the vicinity of the P-wave. Correlation with the electrical activity
of the heart may be necessary for effective operation during periods of maximum uterine
contraction. If the fetus were in normal vertex position the head could become compressed
to the point that the pulse pressure or change in diameter of the vascular system
becomes too small to detect rapidly using optical methods. Thus, the electrical activity
of the fetal heart would provide the additional information for operation under adverse
conditions.
[0079] It is the authors' experience that pretreatment of the spectral or concentration
data can oftentimes improve the analysis precision in the calibration and unknown
analyses as well as increase the robustness of the models. Thus, data pretreatments
including but not limited to centering, scaling, normalizing, taking first or higher
order derivatives, smoothing, Fourier transforming, and/or linearization can all improve
the analysis precision and accuracy. These pretreatments can also improve the robustness
of the model to instrument drift and can improve the transfer of the calibration model
between instruments.
[0080] It is additionally understood by the inventors that the amount of oxygen in the blood
can be recorded as oxygen saturation or partial pressure of oxygen. These two indicators
of oxygen level are strongly correlated, although partial pressure of oxygen will
be affected by pH and the partial pressure of carbon dioxide. Determination of oxygen
saturation is referenced in the specification due to its present use in clinical practice.
[0081] Whereas the drawings and accompanying description have shown and described the preferred
embodiment of the present invention, it should be apparent to those skilled in the
art that various changes may be made in the form of the invention without affecting
the scope thereof.
1. A method of determining non-invasively and in vivo the blood oxygen level in a mammal,
said method comprising the steps of:
a. simultaneously generating a plurality of different wavelengths of light, said wavelengths
being in the range of 500 nm to 1,000 nm;
b. irradiating in vivo and non-invasively blood containing tissue having an unknown
blood oxygen level during the diastolic portion of the cardiac cycle of said mammal
with said wavelengths of light, so that there is differential attenuation of at least
some of said wavelengths by said blood containing tissue as a function of said wavelengths,
said differential attenuation causing intensity variations of said wavelengths incident
from said blood containing tissue as a function of said wavelengths, said tissue and
said unknown blood oxygen level;
c. simultaneously measuring said intensity variations from said blood containing tissue
during said diastolic portion to obtain a diastolic set of intensity variations v.
wavelengths;
d. irradiating in vivo and non-invasively said blood containing tissue during the
systolic portion of said cardiac cycle of said mammal with said wavelengths of light,
so that there is attenuation of at least some of said wavelengths by said blood containing
tissue as a function of said wavelengths, said differential attenuation causing intensity
variations of said wavelengths incident from said blood containing tissue as a function
of said wavelengths, said tissue and said unknown blood oxygen level;
e. simultaneously measuring said intensity variations from said blood containing tissue
during said systolic portion to obtain a systolic set of intensity variations v. wavelengths;
and
f. calculating the value of said unknown blood oxygen level in said blood containing
tissue from said measured intensity variations during said diastolic portion and said
systolic portion of said cardiac cycle utilizing an algorithm and a calibration model,
said algorithm being a multivariate algorithm using 3 or more variables and being
capable of modeling at least some nonlinearities over the entire clinically observed
range of blood oxygen levels, said model being constructed from a set of calibration
samples in which the blood oxygen levels are known, and being a function of said known
oxygen levels and the intensity variations v. wavelengths obtained from irradiating
said set of calibration samples with a plurality of different wavelengths of light,
said wavelengths being in the range of 500 nm to 1,000 nm.
2. The method as set forth in claim 1, further including the step of determining whether
said intensity variations v. wavelengths from said blood containing tissue having
an unknown blood oxygen level represent an outlier.
3. The method as set forth in claim 1, further including the step of pretreatment of
said measured intensity variations, said pretreatment including centering, scaling,
normalizing, taking first or higher order derivatives, smoothing, Fourier transforming
or linearization.
4. The method as set forth in claim 1, wherein said algorithm is selected from the group
including PLS, PCR, CLS, Q-matrix method, cross correlation, Kalman filtering and
MLR.
5. The method as set forth in claim 1, wherein said algorithm has decreased sensitivity
to noise by signal averaging the effects of intensity variations v. wavelengths when
there are more intensities than independent sources of spectral variation.
6. The method as set forth in claim 1, further including the step of determining the
difference between said diastolic set of intensity variations v. wavelengths from
said blood containing tissue and said systolic set of intensity variations v. wavelengths
from said blood containing tissue.
7. The method as set forth in claim 6, wherein said determination of said diastolic portion
and said systolic portion of said cardiac cycle is accomplished by concurrently measuring
the electrical activity of the heart of said mammal.
8. The method as set forth in claim 6, wherein said light incident on said blood containing
tissue is partially absorbed by said tissue and partially diffusely reflected from
said tissue, and wherein at least a portion of said reflected light is subsequently
simultaneously measured.
9. The method as set forth in claim 8, wherein said blood containing tissue is that of
a fetus.
10. The method as set forth in claim 9, wherein the measurement of fetal oxygen level
is made through the chorio-amniotic membrane.
11. The method as set forth in claim 1, further including the step of determining whether
any of said calibration samples from said set of samples is an outlier.
12. A method of determining invasively and in vivo the oxygen level in a sample of blood,
said method comprising the steps of:
a. generating a plurality of different wavelengths of light, said wavelengths being
in the range of 500 nm to 1,000 nm;
b. irradiating said sample with said wavelengths of light so that there is differential
attenuation of at least some of said wavelengths by said sample as a function of said
wavelengths, said differential attenuation causing intensity variations of said wavelengths
incident from said sample as a function of said wavelengths and said unknown blood
oxygen level;
c. measuring said intensity variations from said sample to obtain a set of intensity
variations v. wavelengths;
d. calculating the value of said unknown blood oxygen level in said sample from said
measured intensity variations v. wavelengths utilizing an algorithm and a calibration
model, said algorithm being a multivariate algorithm using 3 or more variables and
being capable of modeling at least some nonlinearities over a blood oxygen level range
corresponding to oxygen saturations of 30% to 100%, said model being constructed from
a set of calibration samples in which the blood oxygen levels are known and being
a function of said known blood oxygen levels and intensity variations v. wavelengths
obtained from irradiating said set of calibration samples with a plurality of different
wavelengths of light, said wavelengths being in the range of 500 nm to 1,000 nm.
13. An oximeter for accurately and precisely determining the blood oxygen level in a mammal
at all levels, including levels corresponding to oxygen saturations of 75% or less,
said oximeter comprising:
a. means for simultaneously generating a plurality of different wavelengths of light,
said wavelengths being in the range of 500 nm to 1,000 nm;
b. means for directing at least a portion all of said wavelengths of light to a section
of blood continuing tissue of a mammal having an unknown oxygen level, said means
for directing including means for coupling to said mammal;
c. means for simultaneously collecting at least a portion of said wavelengths of light
which are directed from said blood containing tissue to said means for collecting,
said means for collecting including said coupling means;
d. means, connected to said means for collecting, for simultaneously measuring the
intensity of each of said wavelengths collected by said means for collecting;
e. means, coupled to said means for measuring, for storing said measured intensity
variations v. wavelengths;
f. means for storing a calibration model, said model being generated by a multivariate
algorithm using 3 or more variables and which is capable of modeling at least some
nonlinearities resulting from irradiation of a set of calibration samples in which
the blood oxygen levels are known and which span the range of variation of all factors
influencing the spectra that are expected to be found in said blood containing tissue,
said model being a function of said known blood oxygen levels from said set of calibration
samples and the intensity variations v. wavelengths obtained from irradiating said
calibration samples with wavelengths of light in the range of 500 nm to 1,000 nm;
g. means for storing said multivariate algorithm which utilizes said calibration model
and said stored intensity variations v. wavelengths for determination of said unknown
blood oxygen level;
h. a microprocessor, coupled to said means for storing said calibration model, said
means for storing said multi-variate algorithm and said means for storing said intensity
variations v. wavelengths, for calculating said unknown blood oxygen level; and
i. means for indicating said calculated blood oxygen level.
14. The oximeter as set forth in claim 13, further including means for determining which
of said intensity variations v. wavelengths correspond to the maximum (systolic) and
minimum (diastolic) expansion of the vascular system of said mammal and means for
determining the differences between said systolic and diastolic intensity variations
v. wavelengths.